On Hypoelliptic Systems with Variable Coefficients
L. R. VOLEVICH
Submitted 1964-01-01 | SovietRxiv: ru-196401.46293 | Translated from Russian

Abstract Generated abstract

This paper studies hypoellipticity for systems of linear differential equations with infinitely differentiable variable coefficients, extending known criteria beyond scalar formally hypoelliptic operators and previously treated special systems such as elliptic, parabolic, and quasi-elliptic cases. A class of square systems is defined by conditions on the determinant, uniform comparability of its associated polynomial norms, and a nondegeneracy estimate on the matrix entries. The proof introduces weighted spaces of generalized vector functions, establishes translation and multiplication lemmas, derives a fundamental a priori estimate, and then uses difference quotients and localization to prove regularity. The main result shows that, for systems satisfying these conditions, every distribution solution is smooth wherever the right-hand side is smooth.

Full Text

MATHEMATICS

L. R. VOLEVICH

ON HYPOELLIPTIC SYSTEMS WITH VARIABLE COEFFICIENTS

(Presented by Academician I. G. Petrovskii, 24 I 1964)

According to L. Schwartz, a differential equation (system) is called hypoelliptic in a domain \(\Omega\) if every generalized solution is infinitely differentiable whenever the right-hand side of the equation has this property.

L. Hörmander \((^1)\) established a criterion for the hypoellipticity of equations (systems) with constant coefficients. Naturally, the problem arose of extending these results to equations with variable coefficients. For a single equation \((^{2,3})\) a naturally broad class was found (formally hypoelliptic operators)\(^*\). As for systems with variable coefficients, hypoellipticity had been proved only for certain classes (elliptic, \(p\)-parabolic, quasi-elliptic \((^7)\)), possessing a special definite principal part. Below we propose a new class of hypoelliptic systems which includes all the above-mentioned systems and equations with variable coefficients.

1. Notation. \(x=(x^1,\ldots,x^n)\) is a point in Euclidean space \(R^n\), \(\xi=(\xi_1,\ldots,\xi_n)\) are variables dual to \(x\) with respect to the scalar product \(x\cdot \xi=x^1\xi_1+\cdots+x^n\xi_n\), \(D=(D_1,\ldots,D_n)\), \(D_k=-i\,\partial/\partial x^k\). If \(\alpha=(\alpha_1,\ldots,\alpha_n)\) is an integer multi-index, then \(D^\alpha=D_1^{\alpha_1}\cdots D_n^{\alpha_n}\), \(|\alpha|=\alpha_1+\cdots+\alpha_n\). A polynomial \(Q(\xi)\) may be written in the form \(\sum a_\alpha \xi^\alpha\) (a differential operator is written similarly as \(Q(x;D)=\sum a_\alpha(x)D^\alpha\)). Put \(Q^{(\alpha)}(\xi)=\partial^{|\alpha|}Q/\partial \xi_1^{\alpha_1}\cdots \partial \xi_n^{\alpha_n}\); \(\widetilde Q(\xi)=\left[\sum_\alpha |Q^{(\alpha)}(\xi)|^2\right]^{1/2}\). By \(\mathscr D,\mathscr D(\Omega)\) we shall denote the space of infinitely differentiable functions in \(R^n\), \(\Omega\), with compact supports, endowed with the natural topology. By \(\mathscr D',\mathscr D'(\Omega)\) are denoted the spaces of generalized functions over \(\mathscr D,\mathscr D(\Omega)\); \(C^\infty(\Omega)\) is the space of infinitely differentiable functions in \(\Omega\).

2. Formulation of the main results. We shall consider the system

\[ \mathscr P(x;D)u(x)=f(x); \tag{1} \]

here \(u(x)=\{u_1(x),\ldots,u_m(x)\}\), \(f(x)=\{f_1(x),\ldots,f_m(x)\}\) are column vectors of height \(m\), and \(\mathscr P(x;D)=\|P_{ij}(x;D)\|_{i,j=1,\ldots,m}\) is a square matrix of linear differential operators with infinitely differentiable coefficients.

Suppose that the following conditions are satisfied:

A. At each fixed point \(x\in\Omega\) the polynomial \(Q(x;\xi)=\det \mathscr P(x;\xi)\) is hypoelliptic (in the sense of \((^1)\)).

B. There exists a constant \(C>0\) such that for all \(x',x''\in\Omega\)

\[ \widetilde Q(x';\xi)<C\widetilde Q(x'';\xi). \]

\(^*\) Somewhat more general hypoelliptic operators are contained in papers \((^{4-6})\).

C. There exist nonnegative numbers \(s_1,\ldots,s_m,\ t_1,\ldots,t_m\), and \(\sigma>0\) such that

\[ \left|P_{ij}^{(\alpha)}(x;\xi)\right|<C[\widetilde Q(x;\xi)]^{t_j-s_i}(1+|\xi|)^{-\sigma|\alpha|}, \]

where

\[ \sum_{i=1}^{m}(t_i-s_i)=1 \]

and \(P_{ij}\equiv 0\) if \(t_j-s_i<0\).

We note that A and B are conditions of formal hypoellipticity of \(\det \mathscr P\), while condition C is an analogue of the “nondegeneracy” condition \((^7)\). As the example in \((^7)\) (p. 4) shows, conditions A and B are not sufficient for hypoellipticity of the system (1).

Main theorem. Let the system (1) in the domain \(\Omega\) satisfy conditions A, B, C. Let \(u\in\mathscr D'(\Omega)\) and \(f\in C^\infty(\Omega)\). Then \(u\in C^\infty(\Omega)\); in other words, the system (1) is hypoelliptic.

We shall prove this theorem according to the scheme proposed in \((^8)\) (for the case of a single equation). As usual, the center of gravity will lie in the derivation of a priori estimates.

3. Some spaces of generalized functions. Denote by \(U^l\) the space of generalized vector-functions \(u=\{u_1,\ldots,u_m\}\), \(u_j\in\mathscr D'\), for which the Fourier transform \(\hat u(\xi)\) is an ordinary locally integrable function and

\[ \|u,U^l\|=\left[\sum_{j=1}^{m}|\hat u_j(\xi)|^2(1+|\xi|)^{2l}\widetilde Q(\xi)^{2t_j}\,d\xi\right]^{1/2}<\infty . \tag{2} \]

Here \(Q(\xi)=Q(0;\xi)=\det\mathscr P(0;\xi)\) \((0\in\Omega)\). Similarly we define the space \(\mathscr F^l\), consisting of vector-functions \(f=\{f_1,\ldots,f_m\}\), \(f_j\in\mathscr D'\), for which

\[ \|f,\mathscr F^l\|=\left[\sum_{i=1}^{m}|\hat f_i(\xi)|^2(1+|\xi|)^{2l}Q(\xi)^{2s_i}\,d\xi\right]^{1/2}<\infty . \tag{3} \]

Lemma 1. For any \(l\), \(u\in U^l\) \((f\in\mathscr F^l)\) if and only if \(u\in U^{l-1}\) \((f\in\mathscr F^{l-1})\), and the expressions

\[ |h|^{-1}\|u_h-u,U^l\|,\qquad |h|^{-1}\|f_h-f,\mathscr F^l\| \]

are uniformly bounded as \(|h|\to0\). Here \(h\) is a vector in \(R^n\); \(u_h,f_h\) are the translates of the generalized functions \(u,f\) by this vector.

Lemma 2. Let \(a\in\mathscr D,\ f\in\mathscr F^l\). Then \(af\in\mathscr F^l\) and the estimate

\[ \|au,\mathscr F^l\|\leq \sup |a(x)|\,\|f,\mathscr F^l\|+C\|f,\mathscr F^{l-\gamma}\|, \tag{4} \]

\(\gamma>0\), holds; the constant \(C>0\) depends on \(a(x)\), but does not depend on \(u\).

The proof of this lemma is based on Lemma 3 and is analogous to the proof of Lemma 2 in \((^8)\).

Lemma 3. Let \(Q(\xi)\) be a hypoelliptic polynomial of order \(\mu\) and let

\[ \mu(\xi)=(1+|\xi|)^l[\widetilde Q(\xi)]^a,\qquad a>0. \]

Then there exists \(\sigma>0\) such that

\[ |\mu(\xi+\eta)-\mu(\xi)|<C(1+|\eta|)^{a\gamma}(1+|\xi|)^{-a\sigma}\mu(\xi). \]

This lemma is based on the fact that for every hypoelliptic polynomial \(Q(\xi)\), for sufficiently large \(\xi\), the inequality \((^2)\)

\[ |Q^{(\alpha)}(\xi)|<C|\xi|^{-\sigma|\alpha|}|Q(\xi)| \tag{5} \]

holds.

  1. The fundamental inequality. The properties B, C of the operator (1) make it possible to write it in the form (cf. (2, 3))

\[ \mathscr{P}(x;D)=\mathscr{P}(D)+\sum_{\omega} a_{\omega}(x)\mathscr{P}_{\omega}(D), \tag{6} \]

where \(a_{\omega}(x)\in C^\infty,\ a_{\omega}(0)=0,\ \mathscr{P}(D)=\mathscr{P}(0;D)\).

If \(\mathscr{P}_{\omega}(D)=\|P_{\omega ij}(D)\|\), then, by virtue of C:

\[ \left|P_{\omega ij}^{(\alpha)}(\xi)\right|\leq C(1+|\xi|)^{-\sigma|\alpha|}\widetilde Q(\xi). \tag{7} \]

Since our aim is to prove the local regularity of solutions of (1), we may assume that \(a_{\omega}(x)\in \mathscr{D}\) and that the quantity \(\delta\)

\[ \delta=\sum_{\omega}\sup |a_{\omega}(x)| \]

is sufficiently small. Under these assumptions we shall establish an estimate.

Theorem 1. Let \(\delta\) be sufficiently small, \(u\in U^l,\ l'<l\). Then there exists a constant \(C>0\) (independent of \(u\)) such that

\[ \|u,U^l\|\leq C\bigl(\|\mathscr{P}(x;D)u,\mathcal F^{\,l'}\|+\|u,U^{l'}\|\bigr). \tag{8} \]

Proof. This theorem must be established for constant coefficients \((\mathscr{P}(x;D)=\mathscr{P}(D))\). The standard passage to variable coefficients is based on representation (6) and Lemma 2. Since smooth finite functions are dense in \(U^l\), we may assume that \(u_j\in\mathscr D,\ j=1,\ldots,m\). Thus, let \(\mathscr{P}(D)u=f\). Passing to the Fourier transform, we obtain the algebraic system

\[ \sum P_{jk}\hat u_k(\xi)=\hat f_j(\xi),\qquad j=1,\ldots,m, \]

from which it follows that

\[ Q(\xi)u_i(\xi)=\sum_{j=1}^{m} P^{ji}(\xi)\hat f_j(\xi), \tag{9} \]

where \(\|P^{ij}(\xi)\|\) is the matrix of algebraic complements of the matrix \(\mathscr P=\|P_{ij}(\xi)\|\). By property C, \(|P^{ji}(\xi)|\leq C\widetilde Q(\xi)^{1-t_j+s_i}\). Since the polynomial \(Q(\xi)\) is hypoelliptic (i.e. (5) is satisfied), for \(l'<l\)

\[ (1+|\xi|)^l\widetilde Q(\xi)\leq C\bigl[(1+|\xi|)^{l'}|Q(\xi)|+(1+|\xi|)^{l'}\widetilde Q(\xi)\bigr]. \]

From these estimates and equality (9) we obtain inequality (8) for \(\mathscr{P}(x;D)=\mathscr{P}(D)\).

  1. Theorem 2 (on the regularity of solutions in the whole space). Let \(u\in U^\lambda\) and \(\mathscr{P}(x;D)u=f\in\mathcal F^l\). Then \(u\in U^l\).

Proof. Let \(\lambda\leq l-1\). We shall show that \(u\in U^{\lambda+1}\). By Lemma 1 it suffices for us to establish the uniform boundedness (in \(h\)) of the norms \(\|\Delta_hu,U^\lambda\|\), where \(\Delta_hu=|h|^{-1}(u_h-u)\). The function \(\Delta_hu\) will satisfy the system

\[ \mathscr{P}(x;D)\Delta_hu=\Delta_hf+\sum \Delta_{-h}a_{\omega}\mathscr{P}_{\omega}(D)u_h. \tag{10} \]

Applying Theorem 1 with \(l=\lambda,\ l'=\lambda-1\), we establish the uniform boundedness of \(\|\Delta_hu,U^\lambda\|\), and together with it also that \(u\in U^{\lambda+1}\). If \(l-1<\lambda<l\), then, applying Theorem 1 with \(l=l-1,\ l'=\lambda-1\), by means of (10) we at once establish the uniform boundedness of \(\|\Delta_hu,U^l\|\), i.e. that \(u\in U^l\). The theorem is proved.

6. Local regularity of solutions.

Let \(u=\{u_1,\ldots,u_m\}\), \(u_j\in \mathcal D'(\Omega)\), where \(\Omega\) is a bounded domain. We shall say that \(u\in U^l_{\mathrm{loc}}(\Omega)\) if \(\varphi u\in U^l\) for every function \(\varphi(x)\in\mathcal D\). The space \(F^l_{\mathrm{loc}}(\Omega)\) is defined analogously.

Lemma 4. Let \(\alpha\) be a multi-index and \(|\alpha|>0\). If \(u\in U^l_{\mathrm{loc}}(\Omega)\), then \(\mathcal P^{(\alpha)}(x;D)u\in F^{l+\sigma}_{\mathrm{loc}}(\Omega)\).

Proof. If \(v\in U^l\), then, by virtue of (7), \(\mathcal P^{(\alpha)}_\omega(D)v\in U^{l+\sigma|\alpha|}\). Using (6) and Lemma 2, we find that \(\mathcal P^{(\alpha)}(x;D)v\in U^{l+\sigma}\). Now let \(u\in U^l_{\mathrm{loc}}(\Omega)\), \(\varphi\in\mathcal D(\Omega)\). Choose a function \(\psi\in\mathcal D(\Omega)\) so that \(\psi(x)=1\) for \(x\in \operatorname{sup} p\,\varphi\). Then
\[ \varphi \mathcal P^{(\alpha)}(x;D)u = \varphi \mathcal P^{(\alpha)}(x;D)\psi u \in U^{l+\sigma}. \]
The lemma is proved.

Theorem 3. Let \(u=\{u_1,\ldots,u_m\}\), \(u_j\in\mathcal D'(\Omega)\); let \(\mathcal P(x;D)u\in F^l_{\mathrm{loc}}(\Omega)\). Then \(u\in U^l_{\mathrm{loc}}(\Omega)\).

Proof. Let \(\Omega'\) be any compact subdomain of \(\Omega\). Then there is such a \(\lambda\) that \(u\in U^\lambda_{\mathrm{loc}}(\Omega)\). We shall show that if \(l\ge \lambda+\sigma\), then \(u\in U^{\lambda+\sigma}_{\mathrm{loc}}(\Omega)\). Indeed, by Leibniz’ formula, for \(\varphi\in\mathcal D(\Omega)\),
\[ \mathcal P(x;D)(\varphi u) = \varphi \mathcal P(x;D)u + \sum D^\alpha \varphi\, \mathcal P^{(\alpha)}(x;D)/|\alpha|! \tag{11} \]
From Lemma 4 it follows that the right-hand side of (11) belongs to \(U^{\lambda+\sigma}\). Then, according to Theorem 2, \(\varphi u\in U^{\lambda+\sigma}\), i.e. \(u\in U^{\lambda+\sigma}_{\mathrm{loc}}(\Omega')\). Repeating these arguments, we find that \(\varphi u\in U^l\), i.e. \(u\in U^l_{\mathrm{loc}}(\Omega')\), and in view of the arbitrariness of \(\Omega'\), \(u\in U^l_{\mathrm{loc}}(\Omega)\). The theorem is proved.

The main theorem formulated above follows immediately from Theorem 3.

Received
21 I 1964

References

¹ L. Hörmander, Acta Math., 94, 161 (1955).
² L. Hörmander, Comm. Pure and Appl. Math., 9, 197 (1958).
³ B. Malgrange, Bull. Soc. Math. France, 85, 283 (1957).
⁴ F. Trèves, Ann. Inst. Fourier, 9, 1 (1959).
⁵ F. Trèves, Am. J. Math., 83, 645 (1961).
⁶ L. Hörmander, Ann. Inst. Fourier, 11, 477 (1961).
⁷ L. R. Volevich, Matem. sborn., 59 (101) (supplementary), 3 (1962).
⁸ J. Peetre, Comm. Pure and Appl. Math., 14, 737 (1961).

Submission history

On Hypoelliptic Systems with Variable Coefficients